2009ApJ...702..154S


Query : 2009ApJ...702..154S

2009ApJ...702..154S - Astrophys. J., 702, 154-170 (2009/September-1)

The 0.8-14.5 µm spectra of mid-l to Mid-T dwarfs: diagnostics of effective temperature, grain sedimentation, gas transport, and surface gravity.

STEPHENS D.C., LEGGETT S.K., CUSHING M.C., MARLEY M.S., SAUMON D., GEBALLE T.R., GOLIMOWSKI D.A., FAN X. and NOLL K.S.

Abstract (from CDS):

We present new 5.2-14.5 µm low-resolution spectra of 14 mid-L to mid-T dwarfs. We also present new 3.0-4.1 µm spectra for five of these dwarfs. These data are supplemented by existing red and near-infrared spectra (∼0.6-2.5 µm), as well as red through mid-infrared spectroscopy of seven other L and T dwarfs presented by Cushing et al. We compare these spectra to those generated from the model atmospheres of Saumon & Marley. The models reproduce the observed spectra well, except in the case of one very red L3.5 dwarf, 2MASS J22244381-0158521. The broad wavelength coverage allows us to constrain almost independently the four parameters used to describe these photospheres in our models: effective temperature (Teff), surface gravity, grain sedimentation efficiency (fsed), and vertical gas transport efficiency (Kzz). The CH4 bands centered at 2.2, 3.3, and 7.65 µm and the CO band at 2.3 µm are sensitive to Kzz, and indicates that chemical mixing is important in all L and T dwarf atmospheres. The sample of L3.5 to T5.5 dwarfs spans the range 1800 K≳ Teff≳1000 K, with an L-T transition (spectral types L7 to T4) that lies between 1400 and 1100 K for dwarfs with typical near-infrared colors; bluer and redder dwarfs can be 100 K warmer or cooler, respectively, when using infrared spectral types. When using optical spectral types, the bluer dwarfs have more typical Teff values as they tend to have earlier optical spectral types. In this model analysis, fsed increases rapidly between types T0 and T4, indicating that increased sedimentation can explain the rapid disappearance of clouds at this stage of brown dwarf evolution. There is a suggestion that the transition to dust-free atmospheres happens at lower temperatures for lower gravity dwarfs.

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Journal keyword(s): stars: individual (2MASS J00361617+1821104, 2MASS J05591914-1404488, 2MASS J08251968+2115521, 2MASS J09083803+5032088, 2MASS J15074769-1627386, 2MASS J22244381-0158521, 2MASS J22443167+2043433, 2MASS J22541892+3123498, DENIS-P J025503.3-470049, SDSS J000013.54+255418.6, SDSS J075840.32+324723.3, SDSS J080531.83+481233.1, SDSS J085758.44+570851.4) - stars: individual (SDSS J105213.50+442255.6AB, SDSS J111009.99+011613.0, SDSS J115553.85+055957.5, SDSS J120747.17+024424.8, SDSS J125453.90-012247.5, SDSS J133148.88-011652.5, SDSS J151643.00+305344.3, SDSS J152039.82+354619.8) - stars: low-mass, brown dwarfs

Simbad objects: 30

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Number of rows : 30
N Identifier Otype ICRS (J2000)
RA
ICRS (J2000)
DEC
Mag U Mag B Mag V Mag R Mag I Sp type #ref
1850 - 2026
#notes
1 2MASS J00001354+2554180 BD* 00 00 13.54488 +25 54 18.0648           T4.5 37 0
2 NAME L 362-29 BC BD* 00 04 34.8671722377 -40 44 06.463544237       19.61 16.88 L5+L5 119 0
3 LSPM J0036+1821 BD* 00 36 16.1118891182 +18 21 10.286665966       18.451 16.053 L3.5 230 0
4 * 54 Psc B BD* 00 39 18.9174 +21 15 16.309           T7.5 86 1
5 DENIS J025503.3-470049 BD* 02 55 03.6927058871 -47 00 51.356903955     22.921 19.906 17.454 L9 170 0
6 2MASSI J0423485-041403 BD* 04 23 48.5763811987 -04 14 03.246502948           L6.5+T2 137 0
7 Cl Melotte 25 OpC 04 30 27.4 +16 46 43           ~ 3309 0
8 2MASS J05591914-1404488 BD* 05 59 19.1872549354 -14 04 49.206913185           T4.5 159 0
9 2MASS J07584037+3247245 BD* 07 58 40.3517739525 +32 47 23.984796389           T0.0+T3.5 54 0
10 2MASS J08053189+4812330 BD* 08 05 31.8496436040 +48 12 33.131831320           L4+T5 51 0
11 2MASSI J0825196+211552 BD* 08 25 19.6125672818 +21 15 51.549358145       21.97 19.22 L7.5V 138 0
12 2MASS J08575849+5708514 BD* 08 57 58.4721442289 +57 08 51.414025854           L7V 57 0
13 2MASS J09083803+5032088 BD* 09 08 38.0091771633 +50 32 08.205341214           L8 54 0
14 2MASS J10210969-0304197 BD* 10 21 09.69240 -03 04 19.7904           T1+T4 79 0
15 2MASS J10521350+4422559 BD* 10 52 13.50504 +44 22 55.9128           L6.5+T1.5 38 0
16 2MASS J11101001+0116130 BD* 11 10 10.01064 +01 16 13.0872           T5.5 86 0
17 DENIS J112639.9-500355 BD* 11 26 39.8047127039 -50 03 54.846166563         17.800 L5.5 52 0
18 2MASS J11555389+0559577 BD* 11 55 53.89032 +05 59 57.7032           L7.5 39 0
19 SDSS J120747.17+024424.8 BD* 12 07 47.17392 +02 44 24.9288           L6.5+T2.5 73 0
20 2MASS J12545393-0122474 BD* 12 54 53.9040607346 -01 22 47.399401142           T2e: 167 0
21 NAME Kelu-1 BD* 13 05 40.1642434199 -25 41 05.712165150         16.85 L2+L3.5 267 0
22 2MASS J13314894-0116500 BD* 13 31 48.9202570553 -01 16 51.118063680           L6V 46 0
23 2MASSW J1507476-162738 BD* 15 07 47.6758255542 -16 27 40.113982846     22.136 18.928 16.579 L5V 216 0
24 2MASS J15164306+3053443 BD* 15 16 43.06536 +30 53 44.3436           L8.0+L9.5 39 0
25 2MASS J15203974+3546210 BD* 15 20 39.74688 +35 46 21.0396           T0.0 33 0
26 HD 154391 PM* 17 01 16.9254812328 +60 38 55.515611040   7.164 6.143     K1III 88 0
27 V* HN Peg B BD* 21 44 28.47168 +14 46 07.7988           T2.5 143 0
28 2MASSW J2224438-015852 BD* 22 24 43.8544128559 -01 58 53.284975671           L4.5V 150 0
29 2MASS J22443167+2043433 BD* 22 44 31.67376 +20 43 43.3020           L6-L8gamma 114 0
30 2MASSI J2254188+312349 BD* 22 54 18.92016 +31 23 49.8300           T5.0 80 0

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